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Approaches to Quantum Gravity

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422 Questions and answers<br />

– A - R. Gambini and J. Pullin:<br />

Indeed, our method of consistent discretizations using as starting point the<br />

Regge action yields a well defined canonical theory for Regge calculus. The<br />

formulation is equivalent <strong>to</strong> the original one classically (apart from some<br />

restrictions on the triangulations that are required <strong>to</strong> have a canonical formulation<br />

that has the same appearance at each point of the manifold). It should<br />

be pointed out that the formulation is canonical but not Hamil<strong>to</strong>nian, the<br />

evolution is given by a discrete canonical transformation instead of a continuous<br />

time evolution generated by a Hamil<strong>to</strong>nian. This is reasonable since<br />

Regge calculus discretizes both space and time. An interesting advantage of<br />

the Hamil<strong>to</strong>nian formulation is that since one naturally restricts the type of<br />

discretizations considered one eliminates the problem of “spikes" and other<br />

pathological structures that may develop in Regge calculus. The disadvantages<br />

include the fact that some of the edges that play the role of Lagrange<br />

multipliers get determined by the evolution equations through complicated<br />

equations that may yield undesired behaviors (like having complex solutions).<br />

In this context the only way of controlling the behavior of these variables is<br />

<strong>to</strong> choose judiciously the initial data. This type of difficulty has led <strong>to</strong> the<br />

construction of a special version of consistent discretizations called “uniform<br />

discretizations” where these problems are eliminated. It might be attractive <strong>to</strong><br />

pursue Regge calculus with this new approach.<br />

• Q - L. Crane - <strong>to</strong> J. Henson:<br />

1. It seems one could equally well use a poset <strong>to</strong> approximate a Lorentzian<br />

manifold in any other dimension than 4. Is there an easy way <strong>to</strong> put conditions<br />

on a causet so that its dimension doesn’t vary from region <strong>to</strong> region?<br />

2. In mathematics there are two very different notions of dimension, one <strong>to</strong>pological<br />

and the other measure theoretic. The best known measure theoretical<br />

definition is Hausdorff dimension, which applies <strong>to</strong> fractals. Do you know of<br />

any approach <strong>to</strong> differentiating these for causets?<br />

– A - J. Henson:<br />

1. Yes, it is true that causets exist which correspond <strong>to</strong> manifolds of other<br />

dimensions. It is possible is estimate the dimension of the approximating<br />

manifold, given the causal set alone, and do as the question suggests. By<br />

different regions one might mean different intervals in the causal set, and the<br />

condition that these dimension estima<strong>to</strong>rs approximately match, and give the<br />

same value (most interestingly 4) in all regions, is a necessary condition for a<br />

causal set <strong>to</strong> be “manifoldlike”.<br />

2. At the discrete level, the causal set does not retain the <strong>to</strong>pological or metric<br />

structures of the continuum, which arise at an effective level. So, the question<br />

of comparison only makes sense for causal sets where a continuum

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